Title: 3D Simulations of Secondary Electron Generation in Diamond and RF Gun Modeling with VORPAL
13D Simulations of Secondary Electron Generation
in Diamond and RF Gun Modeling with VORPAL
Tech-X Corporation
D. A. Dimitrov
Main contributors D. Bruhwiler, R. Busby, D.
Smithe, P. Messmer, J. R. Cary, Ilan Ben-Zvi, T.
Rao, D. Kayran
Work supported by the US Dept. of Energy.
2Collaborators
- Ilan Ben-Zvi
- T. Rao
- D. Kayran
- J. Smedley
- X. Chang
- Q. Wu
- Brookhaven National Lab
- D. L. Bruhwiler
- R. Busby
- D. Smithe
- P. Messmer
- C. Nieter
- J. R. Cary
- VORPAL developers
- Tech-X Corporation
- J. Lewellen
- Argonne National Lab
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3Motivation-I
- A new design for a photoinjector was recently
proposed using diamond as an amplifier of primary
electrons. - The design is very promising for generation of
high-current, high-brightness electron beam. - Experiments have demonstrated the viability of
the concept but the optimal design and parameters
of operation are still being investigated. - Realistic PIC simulations of a photoinjector with
a diamond amplifier are currently not available. - Such simulations are expected to provide valuable
guidance when designing these devices.
4Motivation-II
- Generation of high order modes in an SRF electron
gun with high average and peak current is a
serious concern. - Only a fully electromagnetic code can study this
problem. - The 3D massively parallel particle-in-cell (PIC)
code VORPAL is uniquely suited for this
application. - Investigate how VORPAL compares with PARMELA to
model RF gun properties.
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5Schematic diagram of a secondary emission
enhanced photoinjector (SEEP) courtesy of
Triveni Rao
6Physical Processes Involved
- Elastic scattering - implemented two models
- Isotropic and small angle scattering more
accurate model currently considered - Inelastic scattering for secondary electron and
hole generation that takes band structure into
account - implemented - Electron-hole recombinations
- Acoustic and optical phonon scattering
(inelastic) - Scattering from impurities and defects
- Emission from diamond surfaces taking into
account different electron affinities.
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7Total Elastic and Inelastic Scattering Cross
Sections
8Generation of Secondary Electrons and Holes
- General Monte Carlo algorithm implemented for
scattering processes - Electrons or holes with Ekin gt EG (5.46 eV) can
generate secondaries
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9PDF for the Primary Electron Momentum Change
10Energy Loss Function
11Sampling from the PDF for the Primary Electron
Momentum Change
12Yield of Secondary Electrons is in Fair Agreement
with Previous Simulations
EC 29 (eV) EG 5.46 (eV)
Ep 1000 EC (eV)
Ep 250 EC (eV)
- Two limiting cases considered
- With energy loss to lattice
- No energy loss to lattice
- Averages for Ne are over 200 runs.
13Yield of Secondary Electrons is in Fair Agreement
with Previous Simulations
- Comparison is not under the same conditions.
- Bejata et al. reported
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16VORPAL Geometry Representation Capability
- VORPAL software is able to do curved surfaces
modeling. - Improves accuracy of wakefield and HOM coupling
and propagation through apertures. - Cavity focusing and defocusing effects during
acceleration-deceleration passes.
17VORPAL Provides Second Order Accuracy for 3-D
Accelerating Cavities
- Most codes use stair-step (first order accurate)
boundaries.
18Geometry Representation for the 1.5 Cell RF Gun
Developed in BNL
- 3D VORPAL representation.
- SUPERFISH axially symmetric description.
19Simulation Parameters
- RF field frequency 703.75 MHz
- RF field at cathode surface at t 0 -8.28 MV/m
- RF phase 40 degrees
- RF field amplitude 30 MV/m
- Beer can beam shape with approximately 5 nC total
charge - Beam radius 4 mm
- Beam length 80 ps
Ez (MV/m)
z (cm)
- Multi bunch simulations
- Bunches emitted at each RF period
- 3.5 A average current
- Only at lowest grid resolution currently
20VORPAL Average Kinetic Energy Agrees Well with
PARMELA
- Provides confirmation that accelerating RF fields
are approximately correct.
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21Wakefield effects cause less than 1 variation
in Ekin for multi bunch runs
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22Comparison of RMS Bunch Length - I
- VORPAL results show shorter bunch length but
getting close to the PARMELA result when
increasing the longitudinal grid resolution.
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23Comparison of RMS Bunch Length - II
- The behavior is qualitatively similar.
24Multi Bunch Variation in Zrms
- The wakefieds cause variation in the range
- -1 lt Zrmslt 4
- Most beams are shorter than the first beam by 1
- The 8th beam is longer by 4 .
25VORPAL Shows Qualitatively Similar Transverse RMS
Size Behavior
- The observed transverse rms size was smaller in
VORPAL (the beam was emitted with no thermal
velocities).
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26Wakefield Effects on the Transverse RMS Size
- Consecutive bunches expand transversely by 3
relative to the first bunch.
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27RMS Emittance - I
- Further studies are needed to understand the
differences in the rms emittance, particularly
the effect of wake fields included in VORPAL self
consistently.
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28RMS Emittance - II
- At the exit of the gun, VORPAL shows about 3
times larger emittance. Detailed convergence
simulation at different parameter sets should
provide better understanding of the importance of
different algorithms.
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29Multi Bunch Simulations Show Small Emittance
Increase
- On average, the increase at the exit is 4 .
- Emittance varies from -2 to 4 .
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30Summary and Future Work
- 3D parallel PIC simulations with VORPAL
demonstrated that the code is uniquely suited for
SRF electron gun studies. - Initial simulations and benchmarking of VORPAL
results show quantitative agreement with PARMELA
for some beam parameters and qualitative for
others. - Future studies will focus on
- Completing algorithms for
- electron-hole transport in diamond
- emission of electrons from diamond surfaces
- higher accuracy algorithms,
- simulation studies with PML boundary conditions,
- more accurate treatment of RF fields
- investigation of higher order modes
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31Acknowledgments
This work was supported by the US Department of
Energy, office of Nuclear Physics, under an SBIR
grant and Tech-X Corp.
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